2017
DOI: 10.1063/1.5017505
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Nonlinear dust ion acoustic waves behaviors analysis in warm viscous dusty plasma with trapped ions

Abstract: The nonlinear excitation of a dust ion acoustic (DIA) wave packet in a viscous dusty plasma consisting of Boltzmann distributed electrons, trapped ions, and variable charged dust is investigated. The dependence of the damping rate of the waves on the plasma parameters is discussed via the linear stability analysis. The standard reductive perturbation method is employed to derive the modified Korteweg-de Vries-Burgers equation due to an interplay among the nonlinearity, dispersion, and dissipation effects, and,… Show more

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Cited by 15 publications
(8 citation statements)
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“…In addition, an increase in the constant speed of the reference frame, λ, directly leads to an increase in ϕ0, which means that the energy of the DA solitary wave increases. Now, it would be very interesting to compare our work with that of Patrice et al [ 34 ] Our results, by neglecting the trapping parameter, β, agree with the work of Patrice et al [ 34 ] with cold dust grains have a constant charge. To complement the present work picture, we can examine, in detail, the characteristic of non‐linear DA travelling waves, which have periodic orbits around the equilibrium point normalΘ1.…”
Section: Resultssupporting
confidence: 83%
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“…In addition, an increase in the constant speed of the reference frame, λ, directly leads to an increase in ϕ0, which means that the energy of the DA solitary wave increases. Now, it would be very interesting to compare our work with that of Patrice et al [ 34 ] Our results, by neglecting the trapping parameter, β, agree with the work of Patrice et al [ 34 ] with cold dust grains have a constant charge. To complement the present work picture, we can examine, in detail, the characteristic of non‐linear DA travelling waves, which have periodic orbits around the equilibrium point normalΘ1.…”
Section: Resultssupporting
confidence: 83%
“…[ 23 ] In this study, we can thus simulate a plasma model consisting of negative dust fluid, Maxwellian distributed electrons, and a vortex‐like distribution of trapped ions. The non‐linear excitation of DA waves in the model at hand is governed by the following set of equations [ 26,27,34 ] : nnormaldt+xnnormaldunormald=0, unormaldt+unormaldunormaldxϕx=0, nnormale=expfalse(γϕfalse), nnormali1ϕb(goodbreak−ϕ)3/2+12ϕ2, 2ϕx2=nnormald+δe1δnormalennormale11δnormalennormali. …”
Section: Basic Equationsmentioning
confidence: 99%
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“…Very recently, Tamang and Saha 35 investigated PA superperiodic wave features and its chaotic behaviour in a nonextensive electron–positron–ion plasmas. Not only IA supersoliton but also DIA supersoliton were studied in DPs 36 . The domains of the existence of supersolitons in a DP were estimated by Maharaj et al 37 The propagation of DA supersoliton in a four–component DP was investigated by El‐Wakil et al, 38 and they recognize that the condition of its existence is the consideration of a multicomponent plasma model.…”
Section: Introductionmentioning
confidence: 99%